# Laser diode rate equations

The

laser diode rate equations model the electrical and optical performance of a laser diode. This system ofordinary differential equation s relates the number or density ofphoton s andcharge carrier s (electron s) in the device to the injection current and to device and material parameters such as carrier lifetime, photon lifetime, and the optical gain.The rate equations may be solved by

numerical integration to obtain atime-domain solution, or used to derive a set of steady state or small signal equations to help in further understanding the static and dynamic characteristics of semiconductor lasers.The laser diode rate equations can be formulated with more or less complexity to model different aspects of laser diode behavior with varying accuracy.

**Multimode rate equations**In the multimode formulation, the rate equations model a laser with multiple optical modes. This formulation requires one equation for the carrier density, and one equation for the photon density in each of the

optical cavity modes::$frac\{dN\}\{dt\}\; =\; frac\{I\}\{eV\}\; -\; frac\{N\}\{\; au\_n\}\; -\; sum\_\{mu=1\}^\{mu=M\}G\_mu\; P\_mu$:$frac\{dP\_mu\}\{dt\}\; =\; Gamma\_mu(G\_mu\; -\; frac\{1\}\{\; au\_p\})P\_mu\; +\; eta\_mu\; frac\{N\}\{\; au\_n\}$

where:

M is the number of modes modelled, μ is the mode number, and subscript μ has been added to G, Γ, and β to indicate these properties may vary for the different modes.

**The modal gain**G

_{μ}, the gain of the μ^{th}mode, can be modelled by a parabolic dependence of gainon wavelength as follows::$G\_mu\; =\; frac\{alpha\; N\; [1-(2frac\{lambda(t)-lambda\_mu\}\{deltalambda\_g\})^2]\; -\; alpha\; N\_0\}\{1\; +\; epsilon\; sum\_\{mu=1\}^\{mu=M\}P\_mu\}$

where:α is the gain coefficient and ε is the gain compression factor (see below). λ

_{μ}is the wavelength of the μ^{th}mode, δλ_{g}is the full width at half maximum (FWHM) of the gain curve, the centre of which is given by:$lambda(t)=lambda\_0\; +\; frac\{k(N\_\{th\}\; -\; N(t))\}\{N\_\{th$

where λ

_{0}is the centre wavelength for N = N_{th}and k is the spectral shift constant (see below). N_{th}is the carrier density at threshold and is given by:$N\_\{th\}=N\_\{tr\}\; +\; frac\{1\}\{alpha\; au\_pGamma\}$

where N

_{tr}is the carrier density at transparency.β

_{μ}is given by:$eta\_mu=frac\{eta\_0\}\{1+(2(lambda\_s-lambda\_mu)/deltalambda\_s)^2\}$where

β

_{0}is the spontaneous emission factor, λ_{s}is the centre wavelength for spontaneous emission and δλ_{s}is the spontaneous emission FWHM. Finally, λ_{μ}is the wavelength of the μ^{th}mode and is given by:$lambda\_mu=lambda\_0\; -\; mudeltalambda\; +\; frac\{(n-1)deltalambda\}\{2\}$

where δλ is the mode spacing.

**Gain Compression**The gain term, G, cannot be independent of the high power densities found insemiconductor laser diodes. There are several phenomena which cause the gain to'compress' which are dependent upon optical power. The two main phenomena are

spatial hole burning andspectral hole burning .Spatial hole burning occurs as a result of the standing wave nature of the opticalmodes. Increased lasing power results in decreased carrier diffusion efficiency whichmeans that the stimulated recombination time becomes shorter relative to the carrierdiffusion time. Carriers are therefore depleted faster at the crest of the wave causing adecrease in the modal gain.

Spectral hole burning is related to the gain profile broadening mechanisms suchas short intraband scattering which is related to power density.

To account for gain compression due to the high power densities in semiconductor lasers, the gain equation is modified such that it becomes related to the inverse of the optical power. Hence, the following term in the denominator of the gain equation :

:$1\; +\; epsilon\; sum\_\{mu=1\}^\{mu=M\}P\_mu$

**pectral Shift**Dynamic wavelength shift in semiconductor lasers occurs as a result of the changein refractive index in the active region during intensity modulation. It is possible toevaluate the shift in wavelength by determining the refractive index change of the activeregion as a result of carrier injection. A complete analysis of spectral shift during directmodulation found that the refractive index of the active region varies proportionally to carrier density and hence the wavelength varies proportionally to injected current.

Experimentally, a good fit for the shift in wavelength is given by:

:$deltalambda=kleft(sqrt\{frac\{I\_0\}\{I\_\{th\}-1\; ight)$

where I

_{0}is the injected current and I_{th}is the lasing threshold current.

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